RF inductors - SMD

RF (Radio Frequency) inductors in SMD (Surface Mount Device) form are specialized components used in high-frequency electronic circuits and applications. SMD RF inductors are designed to be mounted directly onto the surface of a circuit board, offering advantages such as space-saving, easy assembly, and compatibility with automated manufacturing processes.
RF inductors are specifically optimized for operation at radio frequency ranges, typically from a few megahertz (MHz) up to several gigahertz (GHz). They are commonly used in RF applications, including RF filters, oscillators, RF amplifiers, impedance matching networks, and wireless communication systems.
SMD RF inductors feature a compact design and are constructed similarly to other inductors. They consist of a coil wound on a core material, but with specific considerations for high-frequency performance and minimizing parasitic effects. These parasitic effects include self-capacitance, series resistance, and interwinding capacitance, which can impact the inductor's performance at high frequencies.
The core materials used in SMD RF inductors are carefully chosen to provide high magnetic permeability, low losses, and stable performance across the desired frequency range. Common core materials for RF inductors include ceramic materials, ferrite, and powdered iron.
SMD RF inductors come in various package sizes and shapes, denoted by standardized codes such as 0402, 0603, or 0805, indicating their dimensions in terms of length and width. This allows for easy integration into surface mount technology and efficient assembly onto circuit boards.
When selecting SMD RF inductors, critical parameters to consider include inductance value, quality factor (Q factor), self-resonant frequency (SRF), and maximum current handling capability. The inductance value determines the component's ability to store energy in its magnetic field, while the Q factor represents its efficiency and ability to maintain high-quality performance. The SRF indicates the frequency at which the inductor starts to exhibit resonance due to its parasitic capacitance. Maximum current handling capability is crucial for ensuring the inductor can withstand the power demands of the RF circuit.
SMD RF inductors are chosen based on specific circuit requirements, such as the desired operating frequency, impedance matching, bandwidth, and available board space. They are essential components in RF systems, contributing to impedance control, filtering, and energy storage functions necessary for reliable and efficient RF signal processing and wireless communication.
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(Ex. GST)(▲▼)		Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
LQW15AN1N3C8ZD


RF Inductors - SMD 1.3 NH
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Murata 19400
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AUD 0.12
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Wirewound0402 (1005 METRIC)Unshielded1.3 nH0.2 nH3.15 A12 mOhms-- 55 C+ 125 C2018 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
LQG15WZ1N5B02D


RF Inductors - SMD
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Murata 19400
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AUD 0.1361
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Multilayer0402 (1005 METRIC)Unshielded1.5 nH0.1 nH1 A40 mOhms-- 55 C+ 125 C2311 GHzStandard1 mm0.6 mm0.5 mm-Air LQGReel , Cut Tape
Hot MLF1005GR39JTD25


RF Inductors - SMD 0402 0.39uH 5% AEC-Q200
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TDK 19400
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AUD 0.1412
Multiples of: 1

Multilayer0402 (1005 METRIC)Shielded390 nH5 %50 mA410 mOhms-- 55 C+ 125 C30600 MHzStandard1 mm0.5 mm0.5 mm-FerriteAEC - Q200MLFReel , Cut Tape
AIMC-0805-4N7S-T


RF Inductors - SMD FIXED IND 4.7NH 400MA 200 MOHM
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ABRACON 19400
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AUD 0.1684
Multiples of: 4000

Multilayer0805 (2012 METRIC)Shielded4.7 nH0.3 nH300 mA200 mOhms - 55 C+ 125 C123.5 GHzStandard2 mm1.25 mm0.85 mm Ceramic AIMC - 0805Reel , Cut Tape
CW100505-68NJ


RF Inductors - SMD 68.0 nH 5% 200 MHz 1.12ohms
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Bourns 19400
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AUD 0.1765
Multiples of: 10000

RF Choke0402 (1005 METRIC)Unshielded68 nH5 %180 mA1.12 Ohms-- 55 C+ 125 C221.62 GHzStandard1 mm0.55 mm0.5 mm-Ceramic CW100505Reel
IWC0603AR27R-3G


RF Inductors - SMD 0603 270nH 2% 170mA
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Laird Performance Materials 19400
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AUD 0.1886
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Wirewound1.8 mm x 1.12 mm x 1.02 mmUnshielded270 nH2 %170 mA2.36 Ohms-- 40 C+ 125 C24900 MHzStandard1.8 mm1.12 mm1.02 mm-Ceramic IWC0603Reel , Cut Tape
B82496C3279A


RF Inductors - SMD 2.7nH 1400mA 0.3nH 1.6x0.8mm SMD
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TDK 19400
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AUD 0.1903
Multiples of: 4000

Wirewound0603 (1608 METRIC)Unshielded2.7 nH0.3 nH1.4 A40 mOhms-- 55 C+ 150 C1410 GHzStandard1.6 mm0.8 mm0.8 mm-CeramicAEC - Q200SIMID - CReel , Cut Tape
AISC-1008-2R2G-T


RF Inductors - SMD FIXED IND 2.2UH 280MA 2.8 OHM
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ABRACON 19400
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AUD 0.3058
Multiples of: 2000

Wirewound1008 (2520 METRIC)Unshielded2.2 uH2 %280 mA2.8 Ohms - 40 C+ 125 C28100 MHzStandard2.92 mm2.79 mm2.29 mm Ceramic AISC - 1008Reel , Cut Tape
MHQ0402PSA2N1CT000


RF Inductors - SMD 01005, 2.1nH +-0.2nH S-HQ SMD RF IND
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TDK 19395
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AUD 0.0525
Multiples of: 1

Multilayer01005 (0402 METRIC)Unshielded2.1 nH0.2 nH400 mA400 mOhms-- 55 C+ 125 C1012.32 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
LQP02TN0N2B02D


RF Inductors - SMD
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Murata 19390
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AUD 0.0485
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Thin Film01005 (0402 METRIC)Unshielded200 pH0.1 nH320 mA500 mOhms-- 55 C+ 125 C1320 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
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